Solid state switching device



April 4, 1967 W. Rt EUBANK 3,312,923

SOLID STATE SWITCHING DEVICE Filed sept. 2v, 1965 2 sheets-.Sheetl 1 F/q. f l

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SOLID STATE SWITCHING DEVICE Filed Sept. 27, 1965 2 Sheets-Sheet 2 A 56 wfg/fm1 United States Patent C) SOLID STATE WITCHING DEVIC William R. Euhank, Troy Township, St. Croix County,

Wis., assigner to Minnesota Mining and Manufacturing Company, St. Paul, Minn., a corporation of Dela- Ware Filed Sept. 27, 1965, Ser. No. 490,515

15 Claims. (Cl. 338-20) This application is a continuation-in-part of my earlier filed application Ser. No. 376,484 tiled June 19, 1964, now abandoned.

This invention relates to new and useful glass compositions containing antimony, sulfur and iodine.

More speciiically, in one embodiment this invention is directed to ternary glasses comprising antirnony, sulfur and iodine, the respective quantities of each such element needed to compose a particular glass composition being variable over predetermined ranges. This embodiment is also directed to a class of glasses containing antimony, sulfur and iodine within the aforementioned class of ternary glasses but containing'a portion of the antimony substituted by one or more of certain other elements from Groups IIIB, IVB, and VB of the Periodic Table and further optionally containing a portion of the sulfur replaced by one or more of certain other elements selected from Group VIB of the Periodic Table. This invention is further directed to methods for making such glasses.

In another embodiment this invention is directed to novel semiconductor devices which use the above-indicated glasses. This embodiment is also directed to methods for making such devices and to methods for making such devices and to methods for using such devices. for using such devices.

In still another embodiment this invention is directed to glass compositions having use in retroretlective structures. This embodiment is also directed to glass structures formed from such glass compositions.

In still another embodiment this invention is directed to opaque high resistivity glasses which, when molten, possess high uidity and ability to wet ceramic materials.

In the following description, references are made to the accompanying drawings wherein:

FIGURE 1 is a ternary diagram of the system antimony-sulfur-iodine showing the glass compositions in atomic weight percentages;

FIGURE 2 shows one embodimentY of a semi-conductor switch construction using a glass composition of this invention;

FIGURE 3 is a vertical sectional view taken across the central portion of another embodiment of a semiconductor switch device of the invention;

FIGURE 4 is a top plan View of the device of FIGURE 3;

FIGUR-E 5 is a view similar to FIGURE 3 but showing a modified form of such device;

FIGURE 6 is a voltage-current plot showing switching characteristics of semi-conductor switch devices of this invention; and

FIGURE 7 shows one embodiment of a circuit diagram suitable for initially activating (i.e. inducing conduction) and then measuring electrical properties of a device of the invention.

.In general, the starting materials employed to produce glasses of this invention either are the uncombined elements or are compounds of two or more such elements. When using uncombined elements, it is generally preferable to employ each in a highly puried and finely divided form. However, largely because of the high volatility of elemental iodine, it is convenient and preferred to employ compounds of iodine in place of iodine itself: for example SbI3.

This embodiment is further directed to circuitry l 3,312,923 Patented Apr. 4, 1967 Finely divided flowers of sulfur are found to be a convenient form of that element to use for making compositions. Granular or powdered analytical grade-antimony is preferably employed. The sulfur and antimony can be preferably prereacted in the ratio to form SbZSg before addition of the ternary component and subsequent formation of a glass, as described below.

In general, one can conveniently use two methods to prepare glass compositions of this invention. One method involves melting starting materials in a closed tube, and the other involves melting starting materials, or remelting a glass formed in the closed tube, in an open tube in order to deposit thin glass layers on a substrate.

The closed tube method for preparing glasses of this invention involves melting the starting materials within a suitable heat resistant sealed tube, as indicated.

The tube after sealing is then preferably suitably mounted for axial rotational movements in a hot zone maintained at a temperature of about 800 C. or higher. Each sealed tube is appropriately thus maintained in such hot zone for about I1/7. to 1 hour or until a homogenous Vliquid melt is obtained. Thereafter, the tube and melt therein are removed from the hot zone and allowed to cool slowly. If any crystallization is visually observed,

the tube and contents are remelted and then rapidly cooled.

When melting in an open tube, one can employ heat resistant glass tubes and deposit in each tube a measured premixed quantity of individually weighed desired starting materials. hot zone maintained at a temperature of from about 600 C. to 700 C. with temperatures about 650 C. being preferred. Though times for the starting materials to melt and become homogeneous vary, they commonly range from about 1/2 to 1 hour, though longer or shorter times may be experienced depending on individual circumstances. Stirring helps promote homogeneity. After a homogeneous melt is obtained, the tube is removed from the hot zone and allowed to cool in air at room temperature. This cooling rate is generally slower than about 10 centigrade per second (10 C./sec.).

If one visually observes any crystallization in the melt as it thus slowly cools within the tube, such tube can be reinserted into the hot zone and the mixture remelted. Then when the hot tube and contents are removed from the hot zone, they are rapidly quenched, as by immersion into water at room temperature or the like, so as to rapidly cool such tube and contents at a rate greater than about centigrade per second 1( 100 C./sec.).

The closed tube method is preferred for studying the glass-forming characteristics of the system studied since possible volatilization losses, resulting in slight compositional changes during melting are thereby eliminated. Also, higher temperatures, by about 100 C., may be employed allowing solution of certain more difficulty soluble components to take place more readily. For practical purposes such as application of thin layers of the glass on a substrate, however, it was necessary to employ the opentube method of melting. In many cases glasses made and characterized by the closed tube method were remelted and obtained as thin layers by the open tube method.

For purposes of this invention in determining whether or not a cooled solid product is a glass (eg. for establishing the glass compositions of FIGURE 1), the following considerations are used:

(l) Presence of conchoidal fracture upon breaking of a sample.

(2) Substantially no birefringence (i.e. double refraction) when a sample is examined under a petrographic microscope (with a glass which is not too opaque for such an examination).

Each such tube is then immersed into a" (3) Substantially no distinct lines indicative of crystal structure when a sample is examined by conventional X-ray powder diffraction techniques.

(4) Gradual softening and final remelting of a sample as its temperature is increased (in contrast to the sharp melting points characteristically observed in the case of crystallized materials).

(5) Forming along continuous [e.g. 2.5 feet (about 1% `meter) or longer] fiber from a sample of molten material as by pulling or suddenly extending in air a sample of molten material smaller than about 1/2 gram before such sample solidifies.

By the use of the foregoing methods and considerations, the phasediagram of FIGURE 1 is prepared. The examples given in Tables I and II below illustrate typical glass compositions which are plotted in terms of atomic percentages of the constituents present and which illus-k t-rate the definition of this phase diagram.

Referring to Table I, nine examples of glass formation within the ternary system of FIGURE 1 are given together with ldetails of composition, electrical and switching properties for each.

Table I illustrates glass compositions within the glass forming region defined by areas A and B of the ternary system shown in FIGURE 1. For instance, Example 1 illustrates a glass derived from a composition consisting of 80 mole percent antimony trisulide and 20 mole percent antimony triiodide (37 atomic percent Sb), While the glass of Example 4 of Table I contains 50 atomic percent antimony (i.e. 13 atomic percent greater than that in the glass of Example 1).

Electrical properties of each glass example are also illustrated in Table I. In general, 0.025 mm. (millimeter) layers of glasses of this invention have initial resistances ranging from about 1012 to 1015 ohms/mm. However, for purposes of clarity in presentation, more detailed explanation of electrical properties is given below.

Table II illustrates glass compositions near the boundary of the glass forming region designated area C of FIG- URE 1. For example, the glass of Example 11 in Table II is just inside the glass forming region outlined in the ternary diagram of FIGURE 1. This glass forms a dark red shiny glass when slowly cooled. On the other hand, the glass of Example 12 of Table II completely devitrifies upon slow cooling showing both birefringence and strong X-,ray powder diffraction lines. Such composition could not be quenched to a stable glass. Hence, it falls outside of `the glass forming region encompassed by this invention (i.e., regions A, B 'and C of FIGURE 1). Note also that'this composition has poor electrical properties.

Specifically, the glass compositions of the examples in Table I were prepared by using both the closed tube and the open tube methods above described. The closed tube technique was used to evaluate the glass forming characteristics of each composition, then each composition is thereafter remelted in an open tube and thin layers den posited on an aluminum strip by dipping. In each example, the procedure followed was to deposit from about 25 to 50 grams of carefully premixed starting materials in the Vbottom of a refractory glass ktest tube. Each tube was then evacuated as with a mechanical rotary vacuum pump to a pressure less than about 10 torr (one torr is equivalent to a pressure of 1 millimeter of mercury, 1/760 atmosphere). Thereafter, each tube was sealed with an oxygen-gas torch, and deposited in an iron pipe adapted to be axially rotated in a tube furnace. Such pipe isV then mounted in the tube furnace. Each sample is then maintained in the furnace at a temperature of about 800 C. for about 321' of an hour, after which the pipe is removed from the furnace and slow cooled- As described above, in the event crystals are formed, the tube is reheated to remelt the contents and then the tube and contents are quenched by immersion into room vtemperature water (about 20 C.). After breaking of the glass tube and separating the sample, the sample is deposited in an open tube and remelted at a temperature somewhat above 600 C. and an aluminum strip immersed into the melt so as to provide a layer approximately 1 mil (about 0.025 mm.) thick on the aluminum. Conveniently such aluminum strip has one surface previously carefully cleaned and is 16 mils (about 0.4 mm.) in thickness and 1/2 inch (about 1.27 cm.) wide and 6 to 8 inches (about 15-20 cm.) long. If the molten glass on the aluminum strip devitrified on cooling, the sample was considered inoperative for purpose of this invention. After dipping and cooling, each so-coated strip is inserted into a sand blasting unit, such as an S. S. White dental abrader, and a glass layer on one side of the aluminum strip completely removed so that subsequent electrical contact can be made with the so-cleaned aluminum surface. Thereafter, the electrical measurements shown were made on the thin layers of glass, as further described hereinafter, when electrical properties of devices of this invention are described.

The glasses of Table II were similarly prepared by the closed tube method and remelted by the open tube method. The preparation procedure followed in each case was substantially the same as that used in the case of the examples of Table I. Finally, the indicated physical measurements were made on each glass sample coating.

In establishing `the ternary diagram for the glass system of this invention it is found to be convenient as a matter of preparatory technique to form glass compositions along either of two joins in the system which a-re labeled in FIGURE 1 as I and II, respectively. These joins are chosen so as to connect two different compounds, namely antimony triiodide and antimony tri-sulde respectively, in the case of join I, and, antimony triiodide and antimony pentasulfide respectively, in the case of join II.

TABLE I (METRIC SYSTEM).-TERNARY, SINGLE PHASE GLASSES OF THE SYSTEM Slo-S-I Composition Atomic Percent Resistance of 0.025 mm. Glass Layer Field (volts per mm.) Required For- (ohms per mm.) Example No.

Sb S I Initial High Low Induced Down- Upswitch 2 Conduction switch 1 Mole Percent Sb2S3, 20 Mole Percent SbIa) X X X 0 3 X10 41 44 15 2 1013 2 1012 1. 2X104 4 104 8X103 1. 2 102 43 42 15 1. 2X1013 1. GX10*2 1. 2X104 4Xl04 8X103 1. 2)(102 50 35 15 3. 2 1012 4X1011 2. 8X10i 2. 8X10* 7. 6 1O3 1. 2x10? 47 43.5 9. 5 I. 6X10l2 3. 2 1011 2)(104 2. 2)(104 7. 6)(103 1. 2)(102 44 38 18 4)(103 2X1()13 2 104 5. 7X1O4 1. 2X104 3. 2)(102 gg 3. 1 Ol 3 Xl 6.2)(104 1.4X104 2. 4 102 0I X10 7. 2 104 1. 6 1 4 2 (67 Mole Percent SbZSa, 33 Mole Percent SbI) X X 0 2x10 43 47. 5 9. 5 3. 3 1012 4 10l2 1. 6X104 3. 2 104 8 l03 2 102 1 Downswitch has reference to the change which occurs in a glass when it switches from its high resistance state to its low resistance state in response to an applied electric field.

2 Upswitch has reference to the change which occurs in a glass when it switches from its low resistance state to its high resistance state in response to an applied electric field.

TABLE I (ENGLISH SYSTElVl).-TERNARY, SINGLE PHASE GLASSES OF THE SYSTEM Sb-S-I Composition Atomic Percent Resistance, l mil Glass Layer, ohms Field (volts per mil) Required For- ExamplevNo.

Sb S I Initial High Low Induced Down- Up- Conduction switch 1 switch 2 (80 Mole Percent SbiSs, 20 Mole Percent SbIs) 41 44 15 5X1011 5 1010 300 1, 000 200 3 43 42 15 3 1011 4X1010 300 1, 000 200 3 50 35 15 8X1010 1 101 700 700 190 3 47 43, 5 9. 5 4X10l 8X10 500 540 190 3 44 38 18 1)(1012 5X1()11 500 1, 380 300 8 40 40 20 8X10l2 2)(1012 200 1, 550 350 6 35 40 25 1. 5)(1013 3 1012 800 1, 800 400 5 (67 Mole Percent SbzSa, 33 Mole Percent SbIs) 1 Downswiteh has reference to the change which occurs in a gloss when it switches from its high resistance state to its low resistance state in response to au applied electric field.

2 Upswitch has reference to the change which occurs in a glass when it switches from its low resistance state to its high resistance state in response to an applied electric field.

TABLE II.-TYPICAL TESTS FOR VITREOUS PROPERTIIODSEQCOMPOSITIONS NEAR BOUNDARIES OF GLASS FORM- For 50 gram Melts For thin Films 1 Example No. Cooling Rate of Visual Appearance Microscopic 2 Examination X-ray Powder State of Material Electrical Melt Diffraction Properties Dark red, shiny glass Traces birefringcnce No lines Glassy Good. Fritted glass No birefringence do Dark glass Birefringenoe Lines Glassy Do. Fritted glass No birefringenee No lines 12 Slo Dull brown mass Birofringenm Strong lines Devitrified Poor.5 Quenched Crystalline powder do 13 Slow- Dull brown mass.. Lincs Devitrified.. Do.

Quenched Fritted glass Faint lines. 14 ow Dull brown mass Birefringenve Lines Glassy Good.

Quenched Fritted glass No birefringenoe No lines 15 ow Dull brown mass Birefrinaenee Strong lines Devitrified Poor.

Quenched Crystalline powder .do do 1 Each film made by dipping a cold aluminum strip into molten glass and rapidly withdrawing; average film thickness was about 1 mil or less. 2 Employing a petrographic microscope (crossed Nicol prisms) with polarized light, tests are made for biretringence (double refraction).

3 Cooling rate of less than 10 C./sec.

4 Cooling rate of greater than 100 C./sec.

5 Inoperative for this invention.

The term iritted has reference to a vitreous granular material;

Surprisingly very stable glasses are found at along join I between about 70 and 90 mole percent Sb2S3. For example, the composition comprising 80 mole percent antimony tri-sulfide and mole percent antimony triiodide gives a completely vitreous, homogenous stable glass which corresponds approximately to composition No. 1, FIGURE 1. Observe-thatin FIGURE 1, Table I and TableIII, respective percentages of antimony, sulfur and iodine are given on an atomic basis. In many compositional studies of the glasses of this invention, this composition No. 1 served as a basis for substitution on a partial atomic basis both forthe antimony and for the sulphur in the glass system.

Referring to FIGURE 1, there is seen fa circular area of glass formation within the ternary system Sb-S-I with a center at point l, FIG. l. Point one designates -a glass made using approximately 80 mole Sb2S3, 20 mole of Sblg. The radius of this circular area of glass formation is aboutV 13 to 14 `atomic percent. The composition of the center point on an atomic basis is 437 at percent Sb, 48 at percent S and 15 atomic percent I. The range of compositions within the circular glass forming area is approximately as follows:

24 to 50 atomic percent sbi13% of point 1, mo. 1 34 to 62 atomic percent Sl l4% of point 1, FIG. 1 2 to 2S atomic percent Ii13% of point l, FIG. 1

capabilities of this ternary system. The procedure in making such substitutions generally involves replacing a predetermined quantity of either or both the antimony and the sulfur inthe mixture of starting materials by suitable precursors which will introduce into the fused or melted product glasses a desired percentage of substitution.

The characteristics of the basic ternary glass are thereby altered in a wide variety of ways by the substitutions given in Table III (below). For example, a given number of atoms up to a given maximum `atomic percent of the antimony can be substituted by other elements, for example 8 atomic percent of phosphorus, Example 16, Table III and so on. Als-o, it is found that, other chalcogcns, such as selenium and tellurium can be substituted for the sulfur on a partial .atomic basis. For,

example, 12 atomic percent of sulfur is substituted by l2 atomic percent of selenium, Example 19, Table III. Resistance data for one mil (about 0.025 mm.) thick glass layers in both the initial, high and low resistance states for each glass `are @also given together with the respective fields in volts per mil (or mm., as the case may be) required for upswitch and for downswitch. In general, the respective maximum substitutions both for antimony .and for sulfur that can be made are given on the basis of the maximum amount that can be employed and still retain glass forming characteristics of the composition. Thus, in the case of germanium, Example 23, Table III, ya range of compositions up to 20 atomic percent germanium were found to form stable glasses. Beyond 20 atomic percent germanium, glasses were not homogeneous, i.e., contained a second phase or showed devitrication, and so are considered outside the scope of this invention.

The glass compositions in Table III are prepared and tested in the same manner as previously described for those glasses shown in Tables I and II with the exception that the additional components were initially added to t-he basic ternary glass compositions in partial substitution for antimony and/or sulfur, in each instance as specifically designated in Table III.

TABLE III (ENGLISH SYSTEM).-SUBSTITUTED GLASSES Composition of substituted Glass (Atomic Percent) Electrical and Switching Properties Resistance, 1 mil Glass Layer Field (volts per mil) Required Example At At (ohms) For- No. At At At Percent Percent Percent Percent Percent (other Other Sb S I (const.) metal) Chalcogcn Induced Up- Down- Initial High Low Conducswitch 1 switch 2 tion 29 48 GX10'I 130 800 2. 8 30 48 8)(10l 500 3, 000 10 500 21 24 1 103 400 4, 200 2 400 37 36 2 l010 800 1,000 6.8 50 37 36 8X10a 500 250 1 25 35 48 7X101 1, 000 500 2. 5 50 29 46 5. 2)(10s 1, 500 1, 600 1. 2 100 21 44 1)(106 170 850 1.8 230 25 45 5. GX10" 250 700 3 350 29 46 5 107 300 900 3 400 29 42. 7 3 104 200 26 0.8 8

1 Upswitch has reference to the change Which occurs in a glass when it switches from its low resistance state toits high resistance state in response to an applied electric field.

2 Downswiteh has reference to the change which occurs in a glass when it switches from its high resistance state to its low resistance state in response to an applied electric field.

Since preparatory procedures, glass determination, and phaseV diagram delineation are all matters Within the skill of those having ordinary familiarity with the art, a further detailed explanation thereof would burden this speci-fication unnecessarily.

The glass product compositions of this invention comprise a ternary glass system and certain substituted glasses based thereon. The ternary glass composition in its broadest aspect comprises antimony, sulfur and iodine in respective amounts as ldefined by the shaded areas A, B and C of FIGURE l in the drawing.

Shaded area A defines ternary glass compositions capable of being formed into a homogeneous solid phase by cooling a liquid composition from a 'temperature -above 600 C. to room temperature at a rate slower than about 10 centigrade per second (10 C./sec.). Integrally imbedded in the cooled solid compositions of area A com- Y positions one can observe no discrete deposits of free antimony metalv greater lthan about 1 micron (about 10-3 mm.) in average individual maximum cross-sectional dimension.

` The ternary glass composition defined by shaded area B of FIGURE 1 of the drawing is capable of being formed into ay homogeneous phase in the same manner as the ternary glass composition defined by shaded area A, that is, by cooling a liquid composition from a temperature above 600 C. to room temperature at a rate slower than about 10 centigrade per second (10 C./sec.). However, compositions defined by area B have integrally imbedded therein, when slow cooled to a solid state, discrete deposits of free antimony metal each of which has an individual average maximum cross-sectional dimension greater than about l micron.

When a glass in shaded area B of the glass forming region of FIGURE 1 is cooled from a molten state, free antimony metal can appear apparently by an exsolution of that metal from the glass. Once molten metal segregates from the molten glass -it settles to the bottom of the melting container, commonly, as a globule of free metal beca-use the molten metal has considerably higher density than that of the molten glass. This globule is readily separated from the glass after cooling. In general, there is no distribution of antimony particles in a solid glass compositions of this invention for purposes of this in` vention can be detected by optical methods. For example, by conventional microscopic techniques involving examining a glass section, one can detect the presence or absence of antimony metal deposits down to about 1 micron in average maximum cross-sectional dimension.

When using the closed tube method, the compositions plotted in area A, FIGURE l, are substantially the same as the starting compositions as weighed on an analytical balance or other suitable weighing device. Although those glasses in area B can contain some free metal as explained above, this `free metal is, however, distinct and separate `from the glassy phase. Although the presence of metal necessarily means that the location of glass compositions in area B, FIGURE 1, is less exact, nevertheless the glass compositions of this Iinvention as deiined by the respective areas A, B and C are considered to be substantially single phased.

C of FIGURE l of the drawing, unlike those glass cornpositions deiined by shaded areas A and B, is capable of being formed into a glassy solid state by cooling a liquid composition from a temperature above 600 C. to room temperature by cooling the liquid composition at a rate faster than about C. per second (100 C./sec.). If a rate much slower than this is used non-vitreous products result. Integrally imbedded within the solid glass ternary compositions defined by shaded area C are substantially no discrete deposits of free antimony metal greater than about 1 micron in average individual maximum cross-sectional dimension.

One of the unusual features of the ternary glass compositions deined by shaded area A of FIGURE 1 is that either or both the antimony and the sulfur can be partially replaced by other elements. Thus, in a given glass composition of this invention the atomic percentV of antimony present can be partially replaced by at least one and less than 4 (preferably only one) of the elements indicated in the following Table IV up to about the maximum atomic percent (Max. At. percent) indicated in said Table IV for each such respective element, provided there is at least 15 atomic percent of antimony remaining in such composition.

TABLE IV Periodic Table Grouping Group IIIB Group IVB Group VB Element Max. At. Element Max. At. Element Max. At.

Percent Percent Percent In Si 10 8 Ge 24 Sn 15 2 Pb 10 Similarly, the atomic percent of sulfur present in ternary glass compositions defined by shaded area A can have the sulfur present partially replaced by an element from Group VlB of the Periodic Table as more speciiically in- Group VIB of the periodic table as more specilically indicated in the following Table V, the maximum Iatomic percent (Max. At. percent) which can be substituted for sulfur being indicated for each such respective element. In addition, it was found that when arsenic substitutes partially for the antimony, as much as 24 atomic percent selenium can simultaneously substitute partially for the sulfur to form a stable, homogeneous glass, Example 18, Table III.

TABLE V Element Max. At. Percent Se (alone) 12 Se (As present) 24 Te (alone 12 In general, all of the glass compositions in this inven-A tion as above described are useful in the manufacture of semiconductor switching devices. A semiconductive solid state switching device of this invention is capable of downswitching from a characteristic high resistance state to a characteristic low resistance state in response to an electric field pulse, and further is capable of upswitching from said low resistance state to said high resistance state in response to `another appropriate electric field pulse. The downswitch pulse required for switching is larger than the upswitch pulse required for switching and the high resistance state is at least about one order in magnitude greater than the low resistance state.

A switching device ofk this invention utilizes a wafer of a glass Aof this invention, either one having a composition as described by the shaded areas A, B, and C of FIGURE 1, or one having a composition in which the antimony and/ or the sulfur is partilly replaced by one or more Iof the respective elements indicated in Tables IV and V ab'ove. Such Ia wafer can have any convenient form. One preferred form is to deposit in a thin layer of glass composition uniformly upon a metal substrate, especially aluminum. Another method is to lap down (e.g. grind or abrade) a s'olid mass of glass composition to a desired thinness, though this method is limited by the thinness of the layer which can be readily produced and handled.

Conveniently and in general, such wafer is in the form of a thin film envelope having a front face and a back face. Each such respective face is commonly separated from the other by an average glass thickness of from about 0.5 to 18 mils (about 0.012 to 0.45 mm.), such `thickness depending upon the characteristics, shape, etc., desired in a given device. The cross-sectional area of each such face is substantially greater than the glass thickness. Other forms of wafer constructions can also be employed, as those skilled in the art will readily appreciate.

Tw'o electrodes are functionally associated with the Wafer, each one with a different surface region thereof. In the case of thin layers, it is convenient to position one electrode on one face of the glass wafer and the other on the opposite face although any suitable arrangement can be used including adjacent positioning of electrodes on a common face. The electrodes can be functionally associated with a wafer in any given way as by employing spring-loaded pointed metal, such as tungsten, contacts. In other cases the electrode on the glass surface may be formed from air drying silver paste. If desired, suitable lead wires of a conductor such as copper 0r aluminum may be soldered to the silver spot employing Woods metal (e.g. wt. percent bismuth, 25 wt. percent lead, 12.5 wt. percent tin, and 12.5 wt. percent cadmium), or other low melting solder.

When the wafer is deposited upon a thin metal substrate or other conductive substrate, such substrate then forms one electrode. Of course, suitable leads are connected to the electrodes to connect the lresulting switching device into a circuit. It will be appreciated that more than two electrodes can be secured to a single wafer construction. The relationship bet-Ween a wafer and each pair of electrodes functionally associated therewith is such that the wafer has a characteristic initial resistance state measured through such electrodes greater than the characteristic high resistance state. The relationship is also such that when a sufficient minimum electric field is applied to such la device (eg. wafer plus electrode pair spaced as described) such device becomes semiconductive as indicated by a change or drop from the characteristic high initial resistance state to a characteristic low resistance state. For example, when a 50 kiloohm resistance is connected in series with such wafer, such resistance serves to limit Vcurrent passing therethrough.

The initial high resistance state, the high resistance state, and the low resistance state, are usually quite constant for a given device. Such resistance states, for purposes of this invention, are conveniently measured in terms of ohms per mil (or ohms per millimeter) of shortest distance between a pair of electrodes used for making such measurements. Thus, the initial resistance characteristically falls in the range of yfrom about 10i5 to 1013 yohms per mil (or about 4X1()6 to 4 1014 ohms per mm.) of shortest distance between electrodes, the high resistance is in the range of from about 104 to 1012 ohms per mil (or about 4 105 to-4 1013 ohms per mm.) of shortest dis- `tance between electrodes and the low resistance` is in the range of from about 102 to 103 ohms per `mil (or about 4 104 Iohms per mm.) of shortest distance between electrodes.

When a switch device is first prepared, it is essentially nonconductive (e.g. it has a characteristic initial high resistance); however, as indicated above, it becomes semiconductive (e.g, falls to a characteristic low resistance state) when a suicient minimum electric eld is applied to the wafer plus, for example, a 50 kiloohm series resistor through a pair of electrodes Whose space is usually, though not necessarily, in the range of from about 0.5 to

l. l. 18 mils (or about 0.012 to 0.45 mm). To render such device semiconductive, electric elds in the range of from about 10 to 103 volts per mil (or about 400 to 4x104 volts per mm.) are commonly'used although it will be appreciated thatv values greater or lower than this can be employed depending upon individual circumstances. This minimum field can be in the form of short bursts or pulses of electric potential. As soon as a device becomes semiconductive, such change can be detected readily by a drop from the characteristic initial resistance state to a lower resistance state which is the characteristic low resistance state for that device.

Once such device is in its characteristic low resistance state the 50 kiloohm series resistor is removed, and when an appropriate upswitch electric field pulse is applied to said device, it switches to its high resistance state. Usually upswitch electric field pulses fall in the range of from about 0.8 to 10 volts per mil (or about 32 to 400 volts per mm.) though potential values above and below this range can be employed depending upon individual circumstances. The minimum pulse duration in terms of time necessary to obtain upswitching similarly varies but commonly appears to be of the order of a few microseconds or less.

One such a device is switched from its low resistance state it assumes its characteristic high resistance state as indicated, but then becomes susceptible to downswitching or returning to its characteristic low resistance state when, for example, a 50 kiloohm resistor is in series and a suitable electric pulse applied. For downswitching, suitable electric field pulses range from about 8 to 500 volts per mil (or about 320 to 2 104 volts per mm.) of time duration from about l microsecond to 1 millisecond, though values greater or smaller than this, of course, may be necessary in individual circumstances.

Usually, there does not appear to be any determinable limit upon the number of times a device may switch `from its high resistance state to its low resistance state. Observe that the high resistance state is always lower than the initial high resistance state.

One embodiment of this invention in the form ofva switching element mounted yfor electrical and switching tests is illustrated in FlGURE 2. The switching element or device 30 comprised of, for example, a one mil (or about 0.025 mm.) layer 31 of glass of Example 1, Table I, on an aluminum substrate 32, is positioned on a support 37 between a pointed tungsten electrode 33 which contacts the aluminum backing and a pointed electrode 34 which contacts the glass layer. The tungsten electrodes are conveniently made of 50 mil (or about 1.25 mm.) wires having U-shaped' bends as illustrated so as to facilitate spring loading or application `of pressure at their points of contact with the switching element. One end of each tungsten electrode is held rigidly by supports 35 and 36, respectively, which serve also as convenient connection points for batteries, pulse generators, measuring meters and other circuit components conventionally used to evaluate the properties of semiconductors.

Another embodiment of a device of this invention' is sho-wn in FIGURES 3 and 4. In these gures, the switching element comprising a glassy layer 38 on an aluminum substrate 39 has fixed lead wire 41 and 42, respectively. Lead wire 41 is attached to the glass surface by soldering to a spot 40 of air drying silver paste using Woods metal or other low melting solder. Lead wire 42 is conveniently attached to the aluminum substrate by spot welding lor other suitable means of joining` metals to aluminum.

Still another embodiment of a device of this invention is shown in FIGURE 5 in which a wafer 43 of the semiconducting glass of compositionV 26, Table III, does not require the support of a metal substrate and because of its relatively low initial resistance can be employed in substantially thicker sizes. 4 Since the initial resistance of this glass is several orders of magnitude lower than that of the previous examples, layers as thick as 20 mils (about 0.5 mm.) can be employed. These thicker wafers 12 can be prepared by conventional semiconductor dicing and lapping techniques. Leads 46 and 47 are attached to the glass wafer 43 of FIGURE 5 by application of air drying silver spots i4 and 45 and soldering with a low melting solder, such as a Woods metal as previously described. The whole assembly, with the exception of the ends of the lead wires, may then be potted in a common` ly used insulating plastic resin 48 for protection and ease of handling.

In general, whether point contact or area contact is made between electrodes and a glass wafer (sometimes called glassy layer or the like for convenience), one achieves the characteristic symmetrical switching capabilities associated `with a semiconductor device of this invention.

FIGURE 6 shows a typical symmetrical switching curve for a device of the invention. To understand this'plot, a series resistance, such as a 50 kiloohm resistor 58, as in FIGURE 7 is placed in the circuit t-o control current and act as a voltage divider. Assume a device 30 of this invention to be in its high resistance state and that a positive electric field is to be applied thereto. The voltage is gradually increased (see FIG. 6) from the origin or zero with little flow of current along the curve 50. At some critical voltage, say 300 volts at point 51 in the illustration of the figure, the device 30 begins to pass current, as shown by the curve 52, and switches rapidly to its low resistance state at point 53.

Next, voltage is reduced to Zero along the low resistance curve 54 and the said series resistance 58 is removed from the circuit. Voltage is again increased positively across device 30 and the low resistance curve 54 results. Voltage-current plot then follows the characteristic low resistance curve 54 to a point 55. The device 30 now again switches to its high resistance state along the negative resistance curve 56 back to high resistance curve 50. This cycle can be repeated indefinitely with either positive or negative voltages. Negative voltages are also illustrated in FIGURE 6. Such use of positive and negative voltages thus produces a symmetrical voltage-current plot.

FIGURE 7 represents one specific embodiment of a circuit useful for switching a device 30 to produce a switching curve such as shown in FIGURE 6. The circuit consists of a 1000-volt, 500-milliampere direct current power supply S7, a SiO-kiloohm series resistor 58, a switch A and the device 30. Voltage 'current characteristics are observed using the pair of terminals 59, 60 and 62, 63 which can be connected, for examlple, to an x-y recorder or a cathode ray oscilloscope. A 1GO-ohm resistor 61 is used for current sampling (eg. measuring current flow in the circuit) as by connecting an x-y recorder or a cathode ray oscilloscope across terminals 62 and 63. For activation of device 30 from its initial high resistance state, switch A increased to a critical value, the resistance of device 33t)l increases suddenly to a high stable resistance state. This high resistance is typically one order of magnitude less than the initial high resistance as indicated above. For downswitching to the low resistance state the procedure is identical to that used for activation except that a lower electric field pulse may be used. Other embodiments of this circuit can be readily constructed.

The glass of Example 1 has an initial resistance when in a 1 mil (about 0.025 mm.) thick vitreous layer of about 5 1012 ohms (assuming about 1 mil (about 0.025 mm.) spacing for electrodes). This glass requires a field of 2000 volts per mil (about 8X104 volts per mm.) to induce conduction. After induced conduction is established,

alaoaa this semiconductor glass has a characteristic low resistance state typically of about 200 ohms for a 1 mil (about 0.025 mm.) thick vitreous layer. Such glass after conduction has thus been induced is capable of downswitching from a characteristic constant high resistance stateto a 'characteristic low resistance state when a voltage pulse of 300 volts is passed therethrough. It is then capable of` upswitching from its characteristic low resistance state to its characteristic high resistance state with a voltage pulse of 8 volts. Y

Another example is the glass of Example 4. Electrical properties of devices of this invention are illustrated by data in tables above. For example, compared to the glass of Example 1, the glass of Example 4 when formed into a device has an initial resistance of about 2 orders of magnitude lower and has a characteristic high resistance of about 8X1010 ohms for a 1 mil (about 0.025 mm.) thick layer. After being rendered conductive, it has a low resistance value of about 500 ohms per mil (about 2x101 ohms per mm.) and is capable of upswitching from this characteristic low resistance state to a characteristic high resistance state of 1010 ohms per mil (about 4X 1011 ohms per mm.) when a voltage pulse of only 3 volts is impressed upon it. It is then capable of downswitching from its characteristic low resistance state with a voltage pulse of 190 volts in a highly repeatable manner.

The electrical characteristics of glasses which have compositions within shaded areas A and C of FIGURE 1 differ from the electrical characteristics of glasses of shaded area B. For example, the glass of Example 1l, which contains no free metal having a particle size larger than about l micron in maximum cross-sectional dimension, has an initial high resistance for a 1 mil (about 0.025 mm.) thick layer of about 1-012 ohms, whereas the glass of Example 4 which falls within area B has an initial high Iresistance Iof about two orders of magnitude less or about 1010 `ohms for a 1 mil (about 0.025 mm.) thick layer.

Switching characteristics differ in glasses of this invention. For example, the glass of Example l requires 2000 volts per mil (about 8 1O4 volts per mm.) to induce conduction versus 700 volts per mil (about 2.8 104 volts per mm.) for the glass of Example 4. Furthermore, the glass of Example` 4 requires lower voltage pulsation for both upswitching and tdownswitching than does the glass of Example l.l

In the semiconductive glasses of this invention -the precise path when conduction is induced is generally not known in an individual device. Hence resistance values instead of resistivity for the various states (initial, high and low resistance, respectively) are used for convenience and are expressed in terms of a l mil (about 0.025 mm.) thickness of glass.

The term wafer as used in this application has a reference to a mass of a glass composition of this invention and is generic to such other terms as layer, ilm, etc. in thin, sheet-like configurations; such term also has reference to not only thin disk-like shapes but also to other physical shapes of generally small dimensions.

By the term symmetrical switching as used in this application, reference is made to a characteristic transition from high to low resistance states (and vice versa) by means of an applied polarity independent electric eld in the form of a pulse or equivalent. This effect is characterized by the fact that a series resistance is required for conversion (i.e. switching) from high to low resistance states.

In addition to their usefulness in switching devices, the

(a) high fluidity at temperatures of from about 600 to Specifically, such opaque glass compositions comprise from about 20 to 30 atomic percent antimony, from about 23 to 33 atomic percent sulfur, from about 10 to 20 atomic percent iodine, from about 14 to 18 atomic percent arsenic, and from about 20 to 28 atomic percent selenium (see, for example, Table 5). In the foregoing composition, the total atomic percentage of elements in any given glass composition is always 100.

Glass compositions for manufacturing glass beads of useful retroreflective structures are produced when a portion of the antimony in the ternary glass of area A, FIG- URE 1 is replaced by arsenic. These glass compositions are characterized by having:

(a) a refractive index l7D of from about 2.7 to 2.85,

(b) the capacity to transmit only light in the range from about 6000 to 7000 A. when struck by -a source of directional polychromatic visible light.

Specifically, such glass compositions comprise from about 20 to 24 atomic percent arsenic, from about 13 to 17 atomic percent antimony, from about 44 to 52 atomic percent sulfur, and from )about 5 to 15 atomic percent iodine, the total atomic percentage tof elements in any given glass composition always being 100.

When these glass compositions are formed into glass structures, such -as glass beads, fibers, flakes, and thin plates, the resulting structures comprise new and useful article of manufacture. In general, these glass structures have thicknesses not exceeding about 2 millimeters and have high optical dispersion Values and high dielectric constants. They are also substantially stable to various types of atmospheric weathering conditions, such as ultra-violet light, humidity, precipitation, etc.

One particularly` useful form of glass element comprises glass beads having average individual diameters not exceeding 4about 100 microns. As those skilled in the art will readily appreciate, the beads can be made by fusing particles of carefully sized cullet which are blown or dropped through a high temperature zone to soften them sufficiently to form transparent spheres by the action of surface tension while moving through a gas such as nitrogen followed by rapid cooling to harden the soproduced spheres without devitriiication. Thecullet can be made by quenching a stream of molten glass in water. The beads can also be made directly from a batch of molten glass.

Fibers can be made by jet-blowing a stream of molten glass. Filaments can be made by drawing molten glass through a die followed by rapid cooling. Thin plates and flakes can be made by casting a thin l-ayer of molten glass upon a lcool steel surface. Small jewelry gems can be made from pieces of this glass. The high refractive index and the high optical dispersion results in high surface sparkle and high internal light reection.

A particularly preferred form for the glass of this invention comprises transparent glass beads having average diameters not exceeding about microns and formed from glass characterized by having a refractive index of at least 2.6, having compositions as above described.

The properties of glass compositions useful in retro- 1'eflective structures are illustrated by Table VI below. These glasses are made by the closed tube method above ydescribed and then formed into cullet. The cullet is then passed through a hot zone and the resulting red beads are thereafter sized.

The term cullet has reference to broken and sized glass, the size range being suitable for the manufacture of glass beads.

TABLE VI.RED RETROREFLEOTIVE GLASSES Composition (Atomic Percent) Relative Light Example No. Transmission, Retroreeetive Refractive percent 1 olor Index 2 Sb As S I 12 27 56 5 50 Red-orange 2. 73 15 24 56 5 -50 `Bright, red 2. 78 15 22 48 15 N50 .do 2.81 18 19 53 l0 50 Dark red 2. 86

1 For glass beads of 50 microns average diameter.

2 Refractive index D measured with petrographic microscope employing apparent depth of focus method.

The embodiments of the invention in which an exclusive property or privilege is claimed as dened as follows:

1. A ternary glass composition comprising antimony, sulfur and iodine inan amount falling within the shaded areas A, B and C of FIGURE 1 in the drawing.

2. A ternary glass composition capable of being formed into a continuous solid phase by cooling trom a liquid phase at temperatures above 600 C. to room temperature at a rate slower than about 10 C. per second, said composition lcompnising antimony, sulfur and iodine in amounts as dened by shaded area A of FIGURE 1 in the drawing.

3. The glass composition of claim 2 characterized by having integrally imbedded therein when a solid state substantially discreet deposits of free antimony metal not greaterrthan about 1 micron in average individual maximum cross-sectional dimension. y 4. A ternary glass composition capable of being formed into a continuous solid phase by cooling from a liquid phase at temperatures above 600 C. to room temperature at a rate slower than about 10 C. per second, said composition comprising antimony, sulfur and iodine in amounts as defined by shaded area B of FIGURE 1 in the drawing.

5. A ternary glass composition capable of being formed into a continuous solid phase by cooling from' a liquid phase at temperatures above 600 C. to room temperature ata rate faster than about 100 C. per second, said composition comprising antimony, sulfur and iodine in :amounts as dened by shaded area C of FIGURE l in the drawing.

6. A yglass composition comprising:

(a) lantimony, sulfur and iodine in respective amounts as defined by the shaded area A of FIGURE `l of the drawings;

(b) the Vatomic percent of antimony present being partially replaced by at least one and less than 4 of the elements and in a respective maximum amount selected from the group consisting of indium up to about l5 atomic percent, silicon up to about 10 atomic percent, germanium up to about 20 atomic percent, tin up to about 15 atomic percent, lead up to about atomic percent, phosphorus up to about 8 atomic percent, arsenic up to about 24 atomic percent and bismuth up to about 2 atomic percent, there being always at least atomic lpercent antimony present;

(c) the atomic vpercent of sulfur present being partially replaced by at least one of the elements and in respective ymaximum amount selected from the group consisting of selenium up to about 12 atomic percent and tellurium up to about 12 atomic percent;

(d) the minimum amount of antimony in any given composition not being less than about 15 atomic percent, and

Y(e) the minimum amount of sulfur in any given com- -position not beibng less than about 24 atomic percent.

7. An opaque glass composition character-ized by hav- (a) high fluidity at temperatures of from about 600 to 650 C.,

(b) ability to wet ceramic materials when in a liquid state, and (c) resistivity greater than about 1012 ohm centimeters at room temperature, said composition comprising:

from about 20 to 30 atomic percent antimony, from about 23 to 33 atomic percent sulfur,

`from about 10 to 20 atomic percent iodine,

from about 14 to 18 atomic percent arsenic, and from about 20 to 28 atomic percent selenium,

the total atomic percentage of elementsV in any given glass composition always being 100.

8. A glass composition suitable for use in glass beads for retroretlective structures characterized by having:

(a) a refractive index 11D of from about 2.7 to 2.85, (b) the capacity to transmit only light in the rangek of from about 6,000 to 7,000 A. when struck by a source of directional polychromatic visible light, said composition comprising:

from about 20 to 24 atomic percent arsenic, from about 13 to 17 atomic percent antimony, from about 44 to 52 atomic percent sulfur, and from about 5 to 15 atomic percent iodine,

the total atomic percentage of elements in any given glass composition always being 1.00.

9. Glass beads characterized by having: (a) a refractive index 11D of from about 2.7 to 2.85, (b) the capacity to transmit only light lin the range of from about 6,000 to 7,000 A. when struck by a source of directional polychromatic light, (c) average individual diameters not exceeding about microns, said glass beads comprising:

from about 20 to 24 atomic percent arsenic, fromy about 13 to 17 atomic percent antimony, from about 44 to 52 atomic,percent sulfur, and from about 5 to 15 atomic percent iodine,

the total atomic percentage of elements in any given glass composition always being 100.

10. A solid state switching device which, when semiconductive, is capable of switching from a characteristic high resistance state to a characteristic low resistance state in response to a downswitch electric eld pulse and further capable of switching from said low resistance state to said high resistance state in response to an upswitch electric eld pulse, said downswitch pulse being larger 17 greater than said characteristic high resistance state; and

(2) when a sufiicient minimum electric iield is applied to said wafer through said electrodes, said wafer becomes semiconductive as indicated by a change from said characteristic initial resistance `state to said characteristic low resistance state.

11. A solid state switching Idevice which, when semiconductive, is capable of switching from la characteristic high resistance state to a -characteristic low resistance state in response to a downswitch electric field pulse and further capable of switching from said low resistance state to said high resistance state in response to an upswitch electric field pulse, said downswitch pulse being larger than said upswitch pulse, said high resistance state being at least about one order in magnitude greater than said low resistance state, said device comprising:

(a) a wafer of a glass composition as defined in claim 6;

(b) two electrodes each one functionally associated with a different surface region of said wafer;

(c) the relationship between said wafer and each of said electrodes, respectively, being such that:

(1) said wafer has a characteristic initial resistance state measured through said electrodes greater than said characteristics high resistance state; and

(2) when a sufiicient minimum electric field is applied to said wafer through said electrodes, said wafer becomes semicon-ductive as indicated by achange from said characteristic initial resistance state to said characteristic low resistance state.

12. A solid state semiconductor switching device comprising:

(a) a wafer of a glass composition as defined in claim (b) said wafer having a front face and a back face;

(c) each such respective face being separated from the other by an average glass thickness of from about 0.5 to 18 mils (about 0.012 to 045 mm.);

(d) the numerical value of the surface area of each such face being substantially greater than the numerical value of such glass thickness;

(e) a pair of electrodes each one associated with a different one of said respective faces and adapted to establish electrical contact therewith;

(f) the relationship between sai-d wafer and each of said electrodes, respectively, being such that the initial resistance measured through said electrodes across said wafer is from about 105 to 1013 ohms per mil (about 4 106 to 4x1014 ohms per mm.) of shortest distance between said electrodes;

(g) when a suicient minimum electric field is applied through said electrodes across said wafer to produce conductivity between said electrical contacts, the low resistance is from about l02 to 103 ohms per mil (about 4 103 to 4 104 ohmsper mm.) of shortest distance between said electrodes;

(h) when an electric field of from about 0.8 to 10 volts per mil (about 32 to 400 volts per mm.) is thereafter applied through said electrodes across said wafer, the resistance across said wafer changes to a high value of from about 101 to 1012 ohms per mil (about 4 105 to 4 10111 ohms per mm.) of shortest distance between sai-d electrodes;

(i) when an electric field of from about 8 to 500 volts per mil (about 320 to 2 101 volts per mm.) is thereafter applied through said electrodes across said wafer, the resistance across said wafer returns to a low value of from about 102 to 103 ohms per mil (about 4X 103 to 4 104 ohms per mm.) of shortest distance between said electrodes;

(j) said initial high resistance before conduction has (b) said wafer having -a front face and a back face;

(c) each such respective face being separated from the other by an average glass thickness of from about 0.5 to 18 mils (about 0.012 to 0.45 mm.);

(d) the numerical va-lue of the surf-ace area of eachl such face being substantially greater than the numerical value of such glass thickness;

(e) a pair of electrodes each one associated with a different one of said respective faces and adapted to establish electrical contact therewith;

(f) the relationship between said wafer and each of said electrodes, respectively, being such that the initial resistance measured through said electrodes across said wafer is from about to 1013 ohms per mil (about 4 106 to 4 1011 ohms per mm.) of shortest distance between said electrodes;

(g) when a suicient minimum electric field is applied through said electrodes across said wafer to lproduce conductivity between said electrical contacts, the low resistance is from about 102 to 103 oh-ms per mil about 4 103 to 4 101 ohms pei-mm.) of shortest distance between said electrodes;

(h) when an electric field of from about 0.8 to 10 Volts per mil (about 32 to 400 volts per mm.) is thereafter applied through said electrodes across said wafer, the resistance across said wafer changes to a high value of from about 104 to 1012 ohms per mil (about 4 105 to 4X 1013 ohms per mm.) of shortest distance between said electrodes;

(i) when 4an electric field of from about 8 to 500 volts per mil (about 32 to 2 104 volts per mm.) is thereafter applied through said electrodes across said wafer, the resistance across said wafer returns to a low value of from about 102 to 103 ohms per mil (about 4 103 to 4 l04 ohms per mm.) of shortest distance between said electrodes;

(j) said initial high resistance being about onerorder of magniutde higher than said high resistance;

(k) said low resistance being about one order of magnitude less than said high resistance; and

(l) the difference between said initial resistance and said low resistance being about at least two orders of magnitude.

14. An electrical switching unit comprising:

(a) a solid state switching device as defined in claim (b) a source of variable electric energy,

(c) means for controlling the quantity of electric energy from said source between limits at least sufficient to switch said device from one resistance state to another,

(d) a resistor in series with said device and adapted to limit the quantity of electric energy from said source applied to said device to a level sufficient to prevent breakdown of said device when said device is passingfrom its characteristic high to its characteristic low resistance state, and

(e) conductor means functionally interconnecting said device, said source, said controlling means, and said resistor. Y

15. A method for controlling which one of two quantities of electric energy shall pass a given point in an electric conductor, there being inserted at such point in said conductor a solid state switching device as defined in 2) claim 13 above, said method comprising the steps of; eld when said device switches from su-ch charac- (a) applying to -said switching device a predetermined teristic high resistance stateto such characteristic 10W low energy electric eld sufcient to switch said l E resistance state. switching element from a characteristic ylow resistance state to a characteristic high resistance state when 5 References Cited by the Examiner i said ydevice is initially in such characteristic low re- UNITED STATES PATENTS sistance state, and

(b) applying to said switching device a predetermined E lrslseretetal* vhigh energy electric field suicient to switch said 3177082 4/1965 M CAVO 106 47 switching device from such characteristic high re- 10 3241009 3/1966 Da ald/t l "t" 106, 47 sistance state to such characteristic low resistance 3249469 5/1966 Stgherr 252 514 state when said element is initially in its high re- 3,258,434 6/1966 Mackenzie et al 106447 sistance state, there being connected in series with ,said device a resistance before said high energy electricfield is so applied sucient to prevent hrcak- 15 RICHARD M' WOOP P'Zmaryxammer down of said `device by said high ener-gy electric W- D- BROOKSASSISIWII Exmlnef.

UNITED STATES PATENT oFFIcE CERTIFICATE OF CORRECTION Patent NO. 3, 312, 923 April 4, 1967 William R. Eubank It is hereby certified that error appears in the above numbered patent requiring correction and that the Said Letters Patent should read as corrected below.

Column l, linesy 31 and 32, strike out and to methods for making such devices"; columns 3 and 4, in TABLE I fifth column, line 9 thereof, for "3.3 l012" read 3.3 l0 3 column 9, line 26, strike out "Group VIB of the periodic table as more specifically in"; column l0, line 66, after "about" insert 4 103 to column ll, line 25, for "One" read Once column l5, line 16, for "as", first occurrence, read are column 18, line 5, (l) should be in the margin under (k) so as to indicate that it is not a subparagraph of (k) same column 18, line 32, before "about" insert Signed and sealed this 21st day of November 1967.

(SEAL) Attest:

EDWARD M.FLETCHER,JR. EDWARD J. BRENNER Attesting Officer Commissioner of Patent 

1. A THERNARY GLASS COMPOSITION COMPRISING ANTIMONY, SULFUR AND IODINE IN AN AMOUNT FALLING WITHIN THE SHADED AREAS A, B AND C OF FIGURE 1 IN THE DRAWING.
 10. A SOLID STATE SWITCHING DEVICE WHICH, WHEN SEMICONDUCTIVE, IS CAPABLE OF SWITCHING FROM A CHARACTERISTIC HIGH RESISTANCE STATE TO A CHARACTERISTIC LOW RESISTANCE STATE IN RESPONSE TO A DOWNSWITHC ELECTRIC FIELD PULSE AND FURTHER CAPABLE OF SWITCHING FROM SAID LOW RESISTANCE STASTE TO SAID HIGH RESISTANCE STATE IN RESPONSE TO AN UPSWITCH ELECTRIC FIELD PULSE, SAID DOWNSWITCH PULSE BEING LARGER THAN SAID UPSWITCH ELECTRIC FIELD PULSE, SAID HIGH RESISTANCE STATE BEING AT LEAST ABOUT ONE ORDER IN MAGNITUDE GREATER THAN SAID LOW RESISTANCE STATE, SAID DEVICE COMPRISING: (A) A WAFER OF A GLASS COMPOSITION AS DEFINED IN CLAIM 1; (B) TWO ELECTRODES EACH ONE FUNCTIONALLY ASSOCIATED WITH A DIFFERENT SURFACE REGION OF SAID WAFER; (C) THE RELATIONSHIP BETWEEN SAID WAFER AND EACH OF SAID ELECTRODES, RESPECTIVELY, BEING SUCH THAT: (1) SAID WAFER HAD A CHARACTERISTIC INITIAL RESISTANCE STATE MEASUREDD THROUGHS SAID ELECTRODES GREATER THAN SAID CHARACTERISTICS HIGH RESISTANCE STATE; AND (2) WHEN A SUFFICIENT MINIMUM ELECTRIC FIELD IS APPLIED TO SAID WAFER THROUGH SAID ELECTRODES SAID WAFER BECOMES SEMICONDUCTOVE AS INDICATED BY A CHANGE FROM SAID CHARACTERISTIC INITIAL RESISTANCE STATE TO SAID CHARACTERISTIC LOW RESISTANCE STATE. 